Patterned multilevel perpendicular magnetic recording media
A patterned perpendicular magnetic recording medium has magnetic islands that contain stacks of individual magnetic cells to provide multilevel recording. Each cell in an island is formed of a material or set of materials to provide the cell with perpendicular magnetic anisotropy and is a single magnetic domain. Each cell is magnetically decoupled from the other cells in its island by nonmagnetic spacer layers. Thus each cell can have a magnetization (magnetic moment) in one of two directions (into or out of the plane of the layer making up the cell), and this magnetization is independent of the magnetization of the other cells in its island. This permits multiple magnetic levels or states to be recorded in each magnetic island.
This application is related to the following concurrently filed co-pending applications, all of which are based on a common specification:
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- “MAGNETIC RECORDING SYSTEM WITH PATTERNED MULTILEVEL PERPENDICULAR MAGNETIC RECORDING MEDIA” (Applicants' Docket HSJ920030214US1)
- “METHOD FOR MAGNETIC RECORDING ON PATTERNED MULTILEVEL PERPENDICULAR MEDIA USING VARIABLE WRITE CURRENT” (Applicants' Docket HSJ920030215US1)
- “METHOD FOR MAGNETIC RECORDING ON PATTERNED MULTILEVEL PERPENDICULAR MEDIA USING THERMAL ASSISTANCE AND FIXED WRITE CURRENT” (Applicants' Docket HSJ920030246US1)
This invention relates to magnetic recording media and systems, such as magnetic recording hard disk drives, and more particular to media and systems with patterned perpendicular magnetic recording media.
BACKGROUND OF THE INVENTIONPatterned magnetic recording media have been proposed to increase the bit density in magnetic recording data storage, such as hard disk drives. In patterned media, the magnetic material is patterned into small isolated blocks or islands such that there is a single magnetic domain in each island or “bit”. The single magnetic domains can be a single grain or consist of a few strongly coupled grains that switch magnetic states in concert as a single magnetic volume. This is in contrast to conventional continuous media wherein a single “bit” may have multiple magnetic domains separated by domain walls. U.S. Pat. No. 5,820,769 is representative of various types of patterned media and their methods of fabrication. A description of magnetic recording systems with patterned media and their associated challenges is presented by R. L. White et al., “Patterned Media: A Viable Route to 50 Gbit/in2 and Up for Magnetic Recording?”, IEEE Transactions on Magnetics, Vol. 33, No. 1, January 1997, 990-995.
Patterned media with perpendicular magnetic anisotropy have the desirable property that the magnetic moments are oriented either into or out of the plane, which represent the two possible magnetization states. It has been reported that these states are thermally stable and that the media show improved signal-to-noise ratio (SNR) compared to continuous (unpatterned) media. However, to achieve patterned media with a bit density of 1 Terabit/in2, a nanostructure array with a period of 25 nm over a full 2.5 inch disk is required. Even though fabrication methods supporting bit densities of up to 300 Gbit/in2 have been demonstrated, large area ultra-high density magnetic patterns with low defect rates and high uniformity are still not available.
The use of multiple level (multilevel) magnetic storage has been proposed, as described in U.S. Pat. No. 5,583,727, but only for continuous (unpatterned) magnetic films and not patterned magnetic islands. However, in multilevel continuous magnetic films the number of magnetic grains, and hence the signal and noise, is divided into the multiple levels, and hence the SNR is degraded.
What is needed is a magnetic recording media and system that takes advantage of both patterned media and multilevel recording.
SUMMARY OF THE INVENTIONThe invention is a patterned perpendicular magnetic recording medium where each magnetic block or island contains a stack of individual magnetic cells. Each cell in an island is formed of a material or set of materials to provide the cell with perpendicular magnetic anisotropy and is a single magnetic domain. Each cell is magnetically decoupled from the other cells in its island by nonmagnetic spacer layers. Thus each cell can have a magnetization (magnetic moment) in one of two directions (into or out of the plane of the layer making up the cell), and this magnetization is independent of the magnetization of the other cells in its island. Therefore the total magnetization integrated over the different cells per island permits multiple magnetic signal levels or states to be recorded in each magnetic island. Because each cell in each island is a single magnetic domain, there is no increase in noise due to the multiple magnetic levels. The number n of magnetic cells stacked in the islands give rise to 2n different readback signal levels. The recording density is thus increased by a factor of 2(n-1).
Each cell in an island has a magnetic coercivity different from the coercivity of the other cells in its island. The magnetic cells can be written (have their magnetizations switched) by an inductive write head capable of writing with multiple write currents, each write current providing a different magnetic write field. Application of a write field greater than the coercivity of only some of the cells but less than the coercivities of the other cells writes just those selected cells in the island. Application of a write field greater than the coercivity of the highest coercivity cell writes all of the cells in the island. The magnetic cells can also be written with thermal assistance by an inductive write head with a fixed write current that provides only a single magnetic write field. Application of the write field without thermal assistance writes only the lower coercivity cell. Application of the same write field but with thermal assistance will write all the cells in the island that have had their temperature raised to close to their Curie temperature because the coercivity of those cells will be below the write field.
The magnetic islands are spaced apart on the substrate by voids or material that does not affect the magnetic properties of the cells and that does not adversely affect writing to the cells. The substrate can be a magnetic recording disk substrate with the islands patterned in concentric tracks or a substrate of the type used in probe-based array storage systems with the islands patterned in an x-y pattern of mutually perpendicular rows.
For a fuller understanding of the nature and advantages of the present invention, reference should be made to the following detailed description taken together with the accompanying figures.
BRIEF DESCRIPTION OF THE DRAWING
FIGS. 8(a) and 8(b) show the two different magnetizations of the probe tip of the MFM probe type inductive head shown in
The spaces 60 define the regions between the magnetic islands and are typically formed of nonmagnetic material, but may be formed of ferromagnetic material provided the material does not adversely affect the signal recording and detection from the magnetic islands that they separate. The magnetic islands can be formed by first lithographically patterning the substrate, depositing the layers making up recording layer 50 over the patterned resist and then removing the resist, leaving the magnetic islands. Alternatively, the magnetic islands can be formed by first depositing the layers making up recording layer 50 on the substrate, lithographically patterning the recording layer, etching the recording layer through the lithographic mask, and then removing the resist, leaving the magnetic islands. In both examples, the spaces 60 in the regions between the islands are voids that may be filled with nonmagnetic material, such as alumina or spin-on glass. A substantially planar surface topography can then be formed. The process would involve first forming the magnetic islands, then depositing alumina to a thickness greater than that required to fill the spaces 60, and then polishing the alumina with a chemical-mechanical polish (CMP) process until the magnetic islands were just exposed. This leaves the alumina in the spaces 60 and the tops of the magnetic islands approximately coplanar.
Patterned media may also be fabricated by ion irradiation through a mask to alter the properties of the irradiated regions. In one example of the patterned media ion irradiation fabrication process, the spaces are formed of magnetic material that does not affect the perpendicular magnetic properties of the magnetic islands. For example, the strong perpendicular magnetic anisotropy of Co/Pt multilayers can be destroyed by ion irradiation through holes in a mask to create regions of magnetic material with in-plane magnetization that serve as the spaces between the magnetic islands of non-irradiated Co/Pt multilayers. Ion irradiation methods of fabricating patterned magnetic recording media are described in the following references: C. Chappert, et al., “Planar Patterned Magnetic Media Obtained by Ion Irradiation,” Science, Vol. 280, Jun. 19, 1998, pp. 1919-922; A. Dietzel et al., “Ion Projection Direct Structuring for Patterning of Magnetic Media”, IEEE Transactions on Magnetics, Vol. 38, No. 5, September 2002, pp. 1952-1954; U.S. Pat. Nos. 6,331,364 and 6,383,597.
As shown by the representative letters A, B, C, D and the arrows in the cells in
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- A: [1,1]
- B: [0,1]
- C: [0,0]
- D: [1,0]
For experimentation, a magnetic thin film was sputter-deposited at room temperature onto an hexagonal array of SiO2 pillars with a diameter of 150 nm and a height of 80 nm. The spacing between the center of the pillars was 300 nm. The pillars were formed by lithographically patterning a SiO2 film formed on a Si substrate. The structure had two perpendicular Co/Pd multilayers separated by a 5 nm thick Pd layer to magnetically decouple the upper and lower multilayers. The composition of the film was as follows:
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- C(40 Å)/Pd(10 Å)/[Co(3.3 Å)/Pd(8.3 Å)]6/Pd(50 Å)/[Co(2.5 Å)/Pd(6.5 Å)]10/Pd(20 Å)/SiO2
Comparing this experimental structure to the schematic of
Magneto-optical Kerr effect (MOKE) hysteresis measurements on a continuous unpatterned section of this structure revealed the distinct switching of each Co/Pd multilayer at different applied fields, as shown in
A magnetic recording experiment was also performed on this island array structure. The structure was fixed on a x-y stage, controlled by piezoelectric drivers with a resolution of less than 2 nm, and scanned at low velocity (approximately 5 μm/s) while in physical contact with the recording head. A conventional longitudinal recording giant magnetoresistive (GMR) read/write head was used with write and read head widths of about 240 nm and 180 nm, respectively. The structure was first dc magnetized in an external perpendicular field of 20 kOe. The recording head was then aligned parallel to the rows of magnetic islands. Although a conventional longitudinal inductive write head generates a write field between its poles that is generally in the plane of the media, in this experiment the perpendicular components of the fringing field from the poles were used to change the magnetization of the perpendicularly magnetized cells in the islands.
In contrast to writing on conventional continuous media, where the bits can be written everywhere on the medium, writing on patterned media requires the synchronization of the square wave write pattern with the island pattern. The island locations can be easily retrieved from the readback signal of the dc-erased magnetized islands, where the minima indicate the trenches or spaces separating the islands, as shown by the top signal in
The experimental results described above were for a multilevel magnetic recording medium wherein the magnetic cells with perpendicular magnetic anisotropy were multilayers of alternating Co/Pd layers. Co/Pt multilayers may also be used. The invention is also fully applicable with other types of magnetic recording materials and structures that provide perpendicular magnetic anisotropy.
The magnetic cells can be formed of a granular polycrystalline cobalt-chromium (CoCr) alloy grown on a special growth-enhancing sublayer that induces the crystalline C-axis to be perpendicular to the plane of the layer, so that the layer has strong perpendicular magnetocrystalline anisotropy. Materials that may be used as the growth-enhancing sublayer for the CoCr granular layer include Ti, TiCr, C, NiAl, SiO2 and CoCr, where Cr is about 35-40 atomic percent.
The magnetic cells can also be formed any of the known amorphous materials that exhibit perpendicular magnetic anisotropy, such as CoSm, TbFe, TbFeCo, and GdFe alloys.
The magnetic cells can also be formed of chemically ordered CoPt, CoPd, FePt, FePd, CoPt3 or CoPd3. Chemically-ordered alloys of CoPt, CoPd, FePt or FePd, in their bulk form, are known as face-centered tetragonal (FCT) L10-ordered phase materials (also called CuAu materials). They are known for their high magnetocrystalline anisotropy and magnetic moment. The c-axis of the L10 phase is the easy axis of magnetization and is oriented perpendicular to the substrate, thus making the material suitable for perpendicular magnetic recording media. Like the Co/Pt and Co/Pd multilayers, these layers have very strong perpendicular anisotropy.
While Pd was used as the spacer layer material in the example described above, essentially any nonmagnetic material can be used, provided it is thick enough to assure that the magnetic cells in the islands are magnetically decoupled. Cu, Ag, Au and Ru are examples of other materials that may be used for the spacer layer.
In perpendicular magnetic recording systems that use pole heads for reading and writing, a “soft” magnetically permeable underlayer is often used on the substrate beneath the magnetic layer to provide a flux return path for the field from the read/write pole head. In perpendicular magnetic recording systems that use ring heads for reading and writing, a soft underlayer may not be necessary. Alloy materials that are suitable for the soft underlayer include NiFe, FeAlSi, FeTaN, FeN, CoFeB and CoZrNb.
Method for Recording on the Multilevel Media Using Variable Write Current
Although
The inductive write head used to record the signal shown in
In the disk drive embodiment of the present invention with the MFM probe as the inductive write head, the cantilever 350 with probe tip 320 is attached to the actuator arm 234 (
The scanning probe system described above and depicted in
While the present invention has been particularly shown and described with reference to the preferred embodiments, it will be understood by those skilled in the art that various changes in form and detail may be made without departing from the spirit and scope of the invention. Accordingly, the disclosed invention is to be considered merely as illustrative and limited in scope only as specified in the appended claims.
Claims
1. A magnetic recording medium comprising:
- a substrate; and
- a plurality of spaced-apart magnetic islands on the substrate, each island comprising at least two stacked magnetic cells, each cell having perpendicular magnetic anisotropy and being separated from the other cells in its island.
2. The medium of claim 1 wherein the magnetic moments of each of two neighboring cells in an island are oriented either parallel or antiparallel.
3. The medium of claim 1 wherein each cell is a single magnetic domain.
4. The medium of claim 3 wherein each cell has a magnetic moment oriented in one of two opposite directions substantially perpendicular to the substrate.
5. The medium of claim 1 wherein each island includes a layer of nonmagnetic material between the stacked cells for separating the cells.
6. The medium of claim 1 wherein the islands are spaced apart by voids.
7. The medium of claim 6 wherein the substrate is patterned into a plurality of pillars and wherein the islands are formed on the pillars.
8. The medium of claim 1 wherein the islands are spaced apart by spacing material formed on the substrate between the islands and having substantially no perpendicular magnetic anisotropy.
9. The medium of claim 8 wherein the spacing material is nonmagnetic.
10. The medium of claim 1 wherein there are only two cells in each island.
11. The medium of claim 1 wherein each cell is a multilayer of alternating layers of a first material selected from the group consisting of Co and Fe and a second material selected from the group consisting of Pt and Pd, said multilayer having magnetic anisotropy substantially perpendicular to the substrate.
12. The medium of claim 1 wherein each cell is formed of a ferromagnetic material comprising one or more of Co, Ni, Fe and alloys thereof.
13. The medium of claim 12 wherein each cell is formed of a ferromagnetic material comprising an alloy of Co and Cr having a magnetocrystalline anisotropy substantially perpendicular to the substrate.
14. The medium of claim 13 wherein each cell is formed directly on a growth enhancing sublayer.
15. The medium of claim 14 wherein the growth enhancing sublayer is formed of a material selected from the group consisting of Ti, TiCr, C, NiAl, SiO2 and CoCr, where Cr is about 35-40 atomic percent in the CoCr sublayer.
16. The medium of claim 1 wherein the cell closest to the substrate in each island has a magnetic coercivity greater than the magnetic coercivity of the other cells in its island.
17. The medium of claim 1 further comprising an underlayer on the substrate beneath the islands.
18. The medium of claim 17 wherein the underlayer is a soft magnetically permeable underlayer of material selected from the group consisting of NiFe, FeAlSi, FeTaN, FeN, CoFeB and CoZrNb.
19. The medium of claim 1 wherein the islands are arranged on the substrate in a plurality of generally concentric circular tracks.
20. The medium of claim 1 wherein the islands are arranged on the substrate in an array of mutually perpendicular rows.
21. A patterned magnetic recording medium comprising a substrate and a plurality of spaced-apart magnetic islands on the substrate, each island comprising at least two stacked magnetic cells, each cell having (a) magnetic anisotropy substantially perpendicular to the substrate, (b) a magnetic moment substantially decoupled from the magnetic moments of neighboring cells in its island, and (c) a magnetic coercivity different from the coercivities of neighboring cells in its island.
22. The medium of claim 21 wherein each island further comprises a spacer layer between neighboring cells for decoupling the magnetic moments of neighboring cells.
23. The medium of claim 21 wherein the islands are spaced apart by voids.
24. The medium of claim 23 wherein the substrate is patterned into a plurality of pillars and wherein the islands are formed on the pillars.
25. The medium of claim 21 wherein the islands are spaced apart by spacing material formed on the substrate between the islands and having substantially no perpendicular magnetic anisotropy.
26. The medium of claim 25 wherein the spacing material is nonmagnetic.
27. The medium of claim 21 wherein there are only two cells in each island.
28. The medium of claim 21 wherein each cell is a multilayer of alternating layers of a first material selected from the group consisting of Co and Fe and a second material selected from the group consisting of Pt and Pd, said multilayer having magnetic anisotropy substantially perpendicular to the substrate.
29. The medium of claim 21 wherein each cell is formed of a ferromagnetic material comprising one or more of Co, Ni, Fe and alloys thereof.
30. The medium of claim 29 wherein each cell is formed of a ferromagnetic material comprising an alloy of Co and Cr having magnetocrystalline anisotropy substantially perpendicular to the substrate.
31. The medium of claim 30 wherein each cell is formed directly on a growth enhancing sublayer.
32. The medium of claim 31 wherein the growth enhancing sublayer is formed of a material selected from the group consisting of Ti, TiCr, C, NiAl, SiO2 and CoCr, where Cr is about 35-40 atomic percent in the CoCr sublayer.
33. The medium of claim 21 further comprising an underlayer on the substrate beneath the islands.
34. The medium of claim 21 wherein the underlayer is a soft magnetically permeable underlayer of material selected from the group consisting of NiFe, FeAlSi, FeTaN, FeN, CoFeB and CoZrNb.
35. The medium of claim 21 wherein the medium is a disk and the islands are arranged on the substrate in a plurality of generally concentric circular tracks.
36. The medium of claim 21 wherein the islands are arranged on the substrate in an array of mutually perpendicular rows.
Type: Application
Filed: Dec 3, 2003
Publication Date: Jun 9, 2005
Patent Grant number: 6947235
Inventors: Manfred Albrecht (Isny-Rohrdorf), Olav Hellwig (Berlin), Guohan Hu (Campbell, CA), Bruce Terris (Sunnyvale, CA)
Application Number: 10/727,826